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Angular Momentum: Single Particle01:10

Angular Momentum: Single Particle

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Angular momentum is directed perpendicular to the plane of the rotation, and its magnitude depends on the choice of the origin. The perpendicular vector joining the linear momentum vector of an object to the origin is called the “lever arm.” If the lever arm and linear momentum are collinear, then the magnitude of the angular momentum is zero. Therefore, in this case, the object rotates about the origin such that it lies on the rim of the circumference defined by the lever arm...
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IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration01:16

IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration

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A covalently bonded heteronuclear diatomic molecule can be modeled as two vibrating masses connected by a spring. The vibrational frequency of the bond can be expressed using an equation derived from Hooke's law, which describes how the force applied to stretch or compress a spring is proportional to the displacement of the spring. In this case, the atoms behave like masses, and the bond acts like a spring.
According to Hooke's law, the vibrational frequency is directly proportional to...
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Atomic Nuclei: Larmor Precession Frequency01:11

Atomic Nuclei: Larmor Precession Frequency

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The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
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Magnetic Moment of an Electron01:23

Magnetic Moment of an Electron

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Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
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Atomic Nuclei: Nuclear Magnetic Moment00:59

Atomic Nuclei: Nuclear Magnetic Moment

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All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
1.1K
π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds01:14

π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds

1.2K
In aromatic compounds, such as benzene, the circulation of (4n + 2) π-electrons sets up a diamagnetic or diatropic ring current around the perimeter of the molecule. This current induces a magnetic field that opposes the external field inside the ring and reinforces it on the outside. The protons in benzene are deshielded and exhibit high chemical shifts in the range 6.5–8.5 ppm. The shielding effect at the center of the ring is evident in complex aromatic molecules, such as...
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Updated: Jun 28, 2025

Spectral and Angle-Resolved Magneto-Optical Characterization of Photonic Nanostructures
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在α-MoO3中的声子伪角动量.

Meiqi Li1, Zhibing Li2,3,4, Huanjun Chen3,4,5

  • 1School of Physics, Sun Yat-sen University, Guangzhou 510275, China.

Nanomaterials (Basel, Switzerland)
|April 12, 2024
PubMed
概括

声子可以在像α-三氧化物 (α-MoO3) 这样的双螺丝旋转对称性晶体中携带伪角运动量. 这一发现指导了循环偏振拉曼实验,并开启了新的应用.

关键词:
螺旋性选择性的拉曼散射.语音 语音 语音 语音伪角动量是一个假角动量.选择规则的选择规则

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科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 固态物理 固态物理
  • 音频电子系统 音频电子系统

背景情况:

  • 最近的研究表明,声子可以携带角动量,主要是在三倍旋转对称的系统中.
  • 具有双螺杆旋转对称性的系统,如α-MoO3,缺乏关于声子角动量的探索.

研究的目的:

  • 为了研究表现出双重螺杆旋转对称性的晶体中声子的伪角运动量.
  • 阐明基于α-MoO3中的伪角运动量保存的循环极化拉曼光谱的选择规则.

主要方法:

  • 理论上研究了声子的伪角运动量.
  • 在循环极化拉曼散射实验中对选择规则的分析.
  • 使用α-三氧化物 (α-MoO3) 作为代表材料的案例研究.

主要成果:

  • 证明了在双螺丝对称晶体中声子伪角动量的存在和性质.
  • 建立了与伪角运动量保存相关的拉曼实验的明确选择规则.
  • 确定了α-MoO3作为研究这些现象的关键材料.

结论:

  • 这项研究介绍了伪角动量作为双螺丝对称系统中声子的关键性质.
  • 为拉曼光谱学提供实验指导,使其能够检测和操纵声子伪角动量.
  • 开辟了在α-MoO3中利用声子伪角动量的新途径,用于高级应用.